Magnetoplasmon excitations in quasi-two-dimensional Rashba spintronic systems:Oscillations, resonances, and energy gaps

We report on the theoretical investigation of plasmon excitations in a quasi-two-dimensional electron gas

(Q2DEG) in the presence of a perpendicular magnetic field and spin-orbit (SO) interaction induced by the

Rashba effect. We derive and discuss the dispersion relations for charge-density excitations within the

framework of Bohm-Pines' random-phase approximation (RPA). The magnetoplasmons in a 2DEG are known to be

characterized by two important properties: (i) the oscillatory behavior of the dispersion curves in the

short wavelength limit (SWL), and (ii) the resonance splitting at the frequency $\omega = n \omega_c$ in

the long wavelength limit (LWL); $n$ ($\ge 2$) being an integer and $\omega_c$ the cyclotron frequency.

Here we study the effect of the Rashba spin-orbit interactions (SOI) on these characteristics in depth.

We observe that the SOI modifies drastically both the oscillatory behavior in the SWL and yields multiple

resonance splittings [at $\omega = (n \pm x_0) \omega_c$] in the LWL. Such resonance splittings make the

spintronic systems potential candidates for quantum-well-based new devices as spin filters. We discuss

the dependence of the magnetoplasmon energy on the propagation vector, the magnetic field, the 2D

charge-density, and the Rashba parameter characterizing the SOI.